TWI540724B - High voltage metal-oxide-semiconductor transistor device - Google Patents

High voltage metal-oxide-semiconductor transistor device Download PDF

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TWI540724B
TWI540724B TW101124598A TW101124598A TWI540724B TW I540724 B TWI540724 B TW I540724B TW 101124598 A TW101124598 A TW 101124598A TW 101124598 A TW101124598 A TW 101124598A TW I540724 B TWI540724 B TW I540724B
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gate
mos transistor
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insulating
depth
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TW101124598A
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TW201403816A (en
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陳勁甫
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聯華電子股份有限公司
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Description

高壓金氧半導體電晶體元件 High voltage MOS transistor

本發明有關於一種高壓金氧半導體(high voltage metal-oxide-semiconductor,以下簡稱為HV MOS)電晶體元件,尤指一種高壓橫向雙擴散金氧半導體(high voltage lateral double-diffused metal-oxide-semiconductor,HV-LDMOS)電晶體元件。 The invention relates to a high voltage metal-oxide-semiconductor (hereinafter referred to as HV MOS) transistor component, in particular to a high voltage lateral double-diffused metal-oxide-semiconductor. , HV-LDMOS) transistor components.

在具有高壓處理能力的功率元件中,雙擴散金氧半導體(double-diffused MOS,DMOS)電晶體元件係持續受到重視。常見的DMOS電晶體元件有垂直雙擴散金氧半導體(vertical double-diffused MOS,VDMOS)與橫向雙擴散金氧半導體(LDMOS)電晶體元件。而LDMOS電晶體元件因具有較高的操作頻寬與操作效率,以及易與其他積體電路整合之平面結構,現已廣泛地應用於高電壓操作環境中,如中央處理器電源供應(CPU power supply)、電源管理系統(power management system)、直流/交流轉換器(AC/DC converter)以及高功率或高頻段的功率放大器等等。LDMOS電晶體元件主要的特徵為具有一低摻雜濃度、大面積的橫向擴散漂移區域,其目的在於緩和源極端與汲極端之間的高電壓,因此可使LDMOS電晶體元件獲得較高的崩潰電壓(breakdown voltage)。 Among power components with high-voltage processing capability, double-diffused MOS (DMOS) transistor components continue to receive attention. Common DMOS transistor components are vertical double-diffused MOS (VDMOS) and lateral double-diffused metal oxide semiconductor (LDMOS) transistor components. LDMOS transistor components are widely used in high-voltage operating environments due to their high operating bandwidth and operating efficiency, as well as planar structures that are easily integrated with other integrated circuits, such as CPU power supply (CPU power). Supply), power management system, AC/DC converter, and high-power or high-band power amplifiers. The main feature of the LDMOS transistor component is that it has a low doping concentration and a large area of lateral diffusion drift region, the purpose of which is to alleviate the high voltage between the source terminal and the drain terminal, thereby enabling a higher breakdown of the LDMOS transistor component. Voltage (breakdown Voltage).

請參閱第1圖,第1圖為一習知HV-LDMOS電晶體元件之剖面示意圖。如第1圖所示,習知HV-LDMOS電晶體元件10係設置於一半導體基底12上,其具有一P型井20、設置於P型井20中的一源極14與一高濃度之P型摻雜區22、一閘極16與一汲極18。汲極18為一高濃度之N型摻雜區,且設置於一N型井30中。此一N型井30即前述之漂移區域,其摻雜濃度與長度影響了HV-LDMOS電晶體元件10的崩潰電壓與導通電阻(ON-resistance,RON)。HV-LDMOS電晶體元件10之閘極16係設置於一閘極介電層40上,且延伸至一場氧化層42上方。 Please refer to FIG. 1. FIG. 1 is a schematic cross-sectional view of a conventional HV-LDMOS transistor device. As shown in FIG. 1, a conventional HV-LDMOS transistor element 10 is disposed on a semiconductor substrate 12 having a P-well 20, a source 14 disposed in the P-well 20, and a high concentration. P-doped region 22, a gate 16 and a drain 18. The drain 18 is a high concentration N-type doped region and is disposed in an N-type well 30. The N-type well 30, that is, the aforementioned drift region, whose doping concentration and length affect the breakdown voltage and ON-resistance (R ON ) of the HV-LDMOS transistor element 10. The gate 16 of the HV-LDMOS transistor component 10 is disposed on a gate dielectric layer 40 and extends over the field oxide layer 42.

由於HV MOS電晶體元件所追求的兩個主要特性為低導通電阻以及高崩潰電壓,且這兩個要求是彼此衝突難以權衡的。因此目前仍需要一種可在高電壓環境下正常運作,且同時滿足低導通電阻以及高崩潰電壓兩個要求的解決途徑。 Since the two main characteristics pursued by HV MOS transistor components are low on-resistance and high breakdown voltage, and these two requirements are conflicting with each other, it is difficult to balance. Therefore, there is still a need for a solution that can operate normally in a high voltage environment while satisfying both low on-resistance and high breakdown voltage.

因此,本發明之一目的係在於提供一具有低導通電阻與高崩潰電壓的HV MOS電晶體元件。 Accordingly, it is an object of the present invention to provide an HV MOS transistor element having low on-resistance and high breakdown voltage.

根據本發明所提供之申請專利範圍,係提供一種HV MOS 電晶體元件,該HV MOS電晶體元件包含有一基底、一設置於該基底上之閘極、分別設置於該閘極兩側之該基底內之一汲極區域與一源極區域、以及一設置於該閘極下方之第一絕緣結構(isolation structure)。值得注意的是,該閘極係完全重疊於該第一絕緣結構。 According to the patent application scope provided by the present invention, an HV MOS is provided The HV MOS transistor device includes a substrate, a gate disposed on the substrate, a drain region and a source region respectively disposed on the substrate on opposite sides of the gate, and a setting a first isolation structure below the gate. It is worth noting that the gate is completely overlapped with the first insulating structure.

根據本發明所提供之申請專利範圍,更提供一種HV MOS電晶體元件,該電晶體元件包含有一基底、一設置於該基底上之閘極、複數個形成於該基底內之漂移區域、複數個形成於該基底內之第一絕緣結構。該閘極係沿一第一方向延伸、該等漂移區域係沿該第一方向排列、而該等第一絕緣結構亦沿該第一方向排列。各該第一絕緣結構係沿一第二方向延伸,且該第二方向垂直於該第一方向。另外,該閘極係覆蓋部分各該漂移區域與部分各該第一絕緣結構,且該閘極下方之該等漂移區域與該等第一絕緣結構係沿該第一方向彼此交錯排列。 According to the patent application scope provided by the present invention, there is further provided an HV MOS transistor device, the transistor device comprising a substrate, a gate disposed on the substrate, a plurality of drift regions formed in the substrate, and a plurality of a first insulating structure formed in the substrate. The gate extends in a first direction, the drift regions are aligned along the first direction, and the first insulating structures are also aligned along the first direction. Each of the first insulating structures extends in a second direction, and the second direction is perpendicular to the first direction. In addition, the gate portion covers each of the drift regions and portions of the first insulating structures, and the drift regions under the gates and the first insulating structures are staggered with each other along the first direction.

根據本發明所提供之HV MOS電晶體元件,係於閘極下方設置與其完全重疊的第一絕緣結構,在不增加導通電阻的前提下增加崩潰電壓。 According to the HV MOS transistor of the present invention, a first insulating structure completely overlapped with the gate is provided under the gate, and the breakdown voltage is increased without increasing the on-resistance.

請參閱第2圖至第4圖,其中第2圖為本發明所提供之 HV MOS電晶體元件之第一較佳實施例之部分佈局圖案示意圖,第3圖至第4圖分別為第2圖中沿A1-A1’與B1-B1’切線所獲得之剖面示意圖。如第2圖至第4圖所示,本較佳實施例所提供之HV MOS電晶體元件100係設置於一基底102,例如一矽基底上。基底102具有一第一導電型態,在本較佳實施例中該第一導電型態為p型。本較佳實施例所提供之HV MOS電晶體元件100包含一閘極120,設置於基底102上,而在基底100內係包含一漂移區域(drift region)106。漂移區域106係包含一第二導電型態,第二導電型態係與第一導電型態互補(complementary),因此在本較佳實施例中第二導電型態為n型,而漂移區域106為一n型漂移區域。在漂移區域106中,係形成有一基體區域108,而基體區域108係包含第一導電型態,故為一p型基體區域。在閘極120兩側之基底102內,係分別設置有一源極區域110與一汲極區域112,源極區域110與汲極區域112皆包含第二導電型態,故為n型源極區域與n型汲極區域。此外如第3圖與第4圖所示,源極區域110係設置於p型基體區域108中,而汲極區域112則設置於n型漂移區域106中。此外,在p型基體區域108中,更設置有一與n型源極區域110互補的p型摻雜區114,且p型摻雜區114係與n型源極區域110電性連接。另外值得注意的是,在第2圖中為強調某些構成元件(element)的空間相對關係,而未繪示出n型源極區域110、n型汲極區域112、p型基體區域108以及p型摻雜 區114等構成元件,但熟習該項技藝之人士應可根據第3圖與第4圖之揭露輕易得知上述構成元件之形成位置,故該等構成元件之空間關係係不再贅述。 Please refer to FIG. 2 to FIG. 4 , wherein FIG. 2 is a partial layout diagram of the first preferred embodiment of the HV MOS transistor component provided by the present invention, and FIG. 3 to FIG. 4 are respectively FIG. A schematic cross-sectional view of the middle edge A 1 -A 1 ' and B 1 -B 1 'tangent. As shown in FIG. 2 to FIG. 4, the HV MOS transistor element 100 provided in the preferred embodiment is disposed on a substrate 102, such as a substrate. The substrate 102 has a first conductivity type, which in the preferred embodiment is p-type. The HV MOS transistor device 100 provided in the preferred embodiment includes a gate 120 disposed on the substrate 102 and including a drift region 106 in the substrate 100. The drift region 106 includes a second conductivity type, and the second conductivity pattern is complementary to the first conductivity pattern. Therefore, in the preferred embodiment, the second conductivity type is n-type, and the drift region 106 It is an n-type drift region. In the drift region 106, a base region 108 is formed, and the substrate region 108 includes a first conductivity type, and thus is a p-type substrate region. In the substrate 102 on both sides of the gate 120, a source region 110 and a drain region 112 are respectively disposed, and the source region 110 and the drain region 112 both include a second conductivity type, so the n-type source region is With n-type bungee area. Further, as shown in FIGS. 3 and 4, the source region 110 is disposed in the p-type body region 108, and the drain region 112 is disposed in the n-type drift region 106. In addition, in the p-type body region 108, a p-type doping region 114 complementary to the n-type source region 110 is further disposed, and the p-type doping region 114 is electrically connected to the n-type source region 110. It is also worth noting that in FIG. 2, the spatial relative relationship of certain constituent elements is emphasized, and the n-type source region 110, the n-type drain region 112, the p-type base region 108, and the like are not illustrated. The p-type doping region 114 and the like constitute elements, but those skilled in the art should be able to easily know the formation positions of the above-described constituent elements according to the disclosures of FIGS. 3 and 4, so the spatial relationship of the constituent elements is no longer Narration.

請同時參閱第2圖至第4圖。本較佳實施例所提供之HV MOS電晶體元件100之閘極120係包含一閘極導電層122、一閘極介電層124、以及形成於閘極導電層122側壁上的側壁子126。且如第2圖所示,設置於基底102上的閘極120係沿一第一方向D1延伸。此外,基底102內更設置有複數個用以提供HV MOS電晶體元件100與其他半導體元件電性隔離的淺溝隔離(shallow trench isolation,STI)104。值得注意的是,本較佳實施例所提供之HV MOS電晶體元件100更包含複數個絕緣結構130,例如複數個STI。如第4圖所示,絕緣結構130之一深度可等於STI 104之深度,但不限於此。各絕緣結構130係彼此平行並沿一第二方向D2延伸,而第二方向D2係如第2圖所示,與第一方向D1相交錯,較佳為互相垂直。更重要的是,絕緣結構130係穿插於n型漂移區域106內,因此在閘極120經過之處,係形成n型漂移區域106與複數個絕緣結構130交錯設置的型態,且n型漂移區域106與絕緣結構130係沿第一方向D1交錯排列。換句話說,閘極120係覆蓋部分各n型漂移區域106與部分各絕緣結構130,且閘極120下方之漂移區域106與第一絕緣結構130係沿第一方向D1彼此交錯排列。如第2圖所示, 在本較佳實施例中,在閘極120下方的絕緣結構130與n型漂移區域106係具有相同的寬度,但不限於此。且絕緣結構130與STI 104可同時製作,但亦不限於此。 Please also refer to Figures 2 to 4. The gate 120 of the HV MOS transistor device 100 provided in the preferred embodiment includes a gate conductive layer 122, a gate dielectric layer 124, and a sidewall spacer 126 formed on the sidewall of the gate conductive layer 122. And as shown in FIG. 2, is provided on the gate electrode 120 on the substrate 102 a line extending in a first direction D 1. In addition, a plurality of shallow trench isolation (STI) 104 for providing electrical isolation between the HV MOS transistor component 100 and other semiconductor components is further disposed in the substrate 102. It should be noted that the HV MOS transistor component 100 provided by the preferred embodiment further includes a plurality of insulating structures 130, such as a plurality of STIs. As shown in FIG. 4, one of the insulating structures 130 may have a depth equal to the depth of the STI 104, but is not limited thereto. The insulating structures 130 are parallel to each other and extend in a second direction D 2 , and the second direction D 2 is interlaced with the first direction D 1 as shown in FIG. 2, preferably perpendicular to each other. More importantly, the insulating structure 130 is interposed in the n-type drift region 106. Therefore, where the gate 120 passes, a pattern in which the n-type drift region 106 and the plurality of insulating structures 130 are alternately arranged is formed, and the n-type drift region 106 and insulating structure 130 along the first direction D 1 lines staggered. In other words, a gate line 120 cover the n-type drift region portion 106 and the insulating portion of each structure 130, 120 and the drift region beneath the gate 106 and the first insulating structure of 130 lines along the first direction D 1 are arranged interleaved with one another. As shown in FIG. 2, in the preferred embodiment, the insulating structure 130 under the gate 120 has the same width as the n-type drift region 106, but is not limited thereto. The insulating structure 130 and the STI 104 can be simultaneously fabricated, but are not limited thereto.

由第2圖至第4圖可知,閘極120下方係交錯形成有n型漂移區域106(以及形成於其內的部分p型基體區域108)與絕緣結構130。如第4圖所示,當閘極120下方形成者為絕緣結構130時,整個閘極結構的閘極導電層122與閘極介電層124係如第4圖所示與絕緣結構130完全重疊。換句話說,閘極120係完全設置於絕緣結構130之區域內,因此本來可形成通道區的部分現在全部被絕緣結構130佔據。然而,當閘極120下方形成者係如第3圖所示為n型漂移區域106以及部分p型基體區域108時,仍可保有通道區域128,並可確保電流可經由n型漂移區域106與通道區域128自汲極區域112到達源極區域110,並在此路徑中達到壓降的目的。更重要的是,由於在平行第二方向D2上,各n型漂移區域106兩側係如第2圖所示皆設置有絕緣結構130,故可減輕n型漂移區域106部分的電場,達到提升崩潰電壓的目的。此外,由於p型基體區域108的角落處(如第3圖中圓圈C所標示)係為最脆弱的p-n交界(p-njunction)處,因此絕緣結構130之深度較佳為大於p型基體區域108之深度,以從兩側夾住p型基體區域108的角落C,而減輕其電場,避免HV MOS電晶體元件100在p型基體區域108的角落C 發生崩潰。 As can be seen from FIGS. 2 to 4, an n-type drift region 106 (and a portion of the p-type base region 108 formed therein) and the insulating structure 130 are alternately formed under the gate 120. As shown in FIG. 4, when the underlying gate 120 is formed as an insulating structure 130, the gate conductive layer 122 and the gate dielectric layer 124 of the entire gate structure are completely overlapped with the insulating structure 130 as shown in FIG. . In other words, the gate 120 is completely disposed within the area of the insulating structure 130, so that portions of the channel region that would otherwise be formed are now fully occupied by the insulating structure 130. However, when the underlying formation of the gate 120 is the n-type drift region 106 and the partial p-type base region 108 as shown in FIG. 3, the channel region 128 can still be retained, and current can be ensured via the n-type drift region 106. The channel region 128 reaches the source region 110 from the drain region 112 and achieves a voltage drop in this path. More importantly, since the insulating structures 130 are disposed on both sides of the n-type drift regions 106 as shown in FIG. 2 in the parallel second direction D 2 , the electric field of the n-type drift region 106 can be alleviated. Increase the purpose of the breakdown voltage. In addition, since the corner of the p-type base region 108 (as indicated by the circle C in FIG. 3) is the most fragile pn junction, the depth of the insulating structure 130 is preferably larger than the p-type base region. The depth of 108 is such that the corner C of the p-type base region 108 is sandwiched from both sides to reduce the electric field thereof, and the HV MOS transistor element 100 is prevented from collapsing at the corner C of the p-type base region 108.

因此,根據本第一較佳實施例所提供的HV MOS電晶體元件100,係藉由閘極120下方交錯設置的n型漂移區域106與絕緣結構130減輕n型漂移區域106電場,故可在不增加導通電阻的前提下成功提升崩潰電壓。 Therefore, the HV MOS transistor element 100 according to the first preferred embodiment reduces the electric field of the n-type drift region 106 by the n-type drift region 106 and the insulating structure 130 staggered under the gate 120. Successfully increase the breakdown voltage without increasing the on-resistance.

請參閱第5圖至第7圖,其中第5圖為本發明所提供之HV MOS電晶體元件之一第二較佳實施例之部分佈局圖案示意圖,第6圖至第7圖分別為第5圖中沿A2-A2’與B2-B2’切線所獲得之剖面示意圖。如第5圖至第7圖所示,本較佳實施例所提供之HV MOS電晶體元件200係設置於一基底202上。基底202具有一第一導電型態,在本較佳實施例中該第一導電型態亦為p型。本較佳實施例所提供之HV MOS電晶體元件200包含一閘極220,設置於基底202上,而在基底200內係包含一漂移區域206。漂移區域206係包含一第二導電型態,第二導電型態係與第一導電型態互補,因此在本較佳實施例中第二導電型態亦為n型。在n型漂移區域206中,係形成有一基體區域208,而基體區域208係包含第一導電型態,故為一p型基體區域。在閘極220兩側之基底202內,係分別設置有一源極區域210與一汲極區域212,源極區域210與汲極區域212皆包含第二導電型態。此外如第6圖與第7圖所示,源極區域210係設置於p型基體區域 208中,而汲極區域212則設置於n型漂移區域206中。此外,在p型基體區域208中,更設置有一與n型源極區域210互補的p型摻雜區214,且p型摻雜區214係與n型源極區域210電性連接。另外值得注意的是,在第5圖中為強調某些構成元件(element)的空間相對關係,而未繪示出n型源極區域210、n型汲極區域212、p型基體區域206以及p型摻雜區214等構成元件,但熟習該項技藝之人士應可根據第6圖與第7圖之揭露輕易得知上述構成元件之形成位置,故該等構成元件之空間關係則不再贅述。 Please refer to FIG. 5 to FIG. 7 , wherein FIG. 5 is a partial layout diagram of a second preferred embodiment of the HV MOS transistor component provided by the present invention, and FIG. 6 to FIG. 7 are respectively 5th. A schematic cross-sectional view taken along the line A 2 -A 2 ' and B 2 -B 2 ' in the figure. As shown in FIG. 5 to FIG. 7, the HV MOS transistor element 200 provided in the preferred embodiment is disposed on a substrate 202. The substrate 202 has a first conductivity type, which in the preferred embodiment is also p-type. The HV MOS transistor device 200 provided in the preferred embodiment includes a gate 220 disposed on the substrate 202 and including a drift region 206 in the substrate 200. The drift region 206 includes a second conductivity type, and the second conductivity pattern is complementary to the first conductivity type. Therefore, in the preferred embodiment, the second conductivity type is also n-type. In the n-type drift region 206, a matrix region 208 is formed, and the substrate region 208 includes a first conductivity type, and thus is a p-type substrate region. In the substrate 202 on both sides of the gate 220, a source region 210 and a drain region 212 are respectively disposed, and the source region 210 and the drain region 212 both include a second conductivity type. Further, as shown in FIGS. 6 and 7, the source region 210 is disposed in the p-type body region 208, and the drain region 212 is disposed in the n-type drift region 206. In addition, in the p-type body region 208, a p-type doping region 214 complementary to the n-type source region 210 is further disposed, and the p-type doping region 214 is electrically connected to the n-type source region 210. It is also worth noting that in FIG. 5, the spatial relative relationship of certain constituent elements is emphasized, and the n-type source region 210, the n-type drain region 212, the p-type substrate region 206, and the like are not illustrated. The p-type doping region 214 and the like constitute an element, but those skilled in the art should be able to easily know the formation position of the above-mentioned constituent elements according to the disclosures of FIGS. 6 and 7, so that the spatial relationship of the constituent elements is no longer Narration.

請同時參閱第5圖至第7圖。本較佳實施例所提供之HVMOS電晶體元件200之閘極220係包含一閘極導電層222、一閘極介電層224、以及形成於閘極導電層222側壁上的側壁子226。且如第5圖所示,設置於基底202上的閘極220係沿一第一方向D1延伸。此外,基底202內更設置有複數個用以提供HV MOS電晶體元件200與其他半導體元件電性隔離的STI 204。值得注意的是,本較佳實施所提供之HV MOS電晶體元件200更包含複數個絕緣結構230,例如複數個STI。值得注意的是,本較佳實施例所提供之絕緣結構230係分別由一第一絕緣結構230a與一第二絕緣結構230b所構成。如第5圖所示,絕緣結構230的各個第一絕緣結構230a係沿一第二方向D2延伸,而第二方向D2係如第5圖所示,與第一方向D1相交錯,較佳為互相垂直。更重要的是,第 一絕緣結構230a係穿插於n型漂移區域206內,因此在閘極220經過之處,係形成n型漂移區域206與複數個第一絕緣結構230a交錯設置的型態,且n型漂移區域206與第一絕緣結構230a係沿第一方向D1交錯排列。換句話說,閘極220係覆蓋部分各n型漂移區域206與部分各絕緣結構230,且閘極220下方之漂移區域206與第一絕緣結構230係沿第一方向D1彼此交錯排列。如第5圖所示,在本較佳實施例中,第一絕緣結構230a與n型漂移區域106係具有相同的寬度,但不限於此。絕緣結構230的第二絕緣結構230b係沿第一方向D1延伸,且設置於閘極220下方靠近汲極區域212之一側。另外,如第5圖所示,第二絕緣結構230b係設置於第一絕緣結構230a的一側,而與部分的各第一絕緣結構230a重疊且實體上(physically)連接。更重要的是,各第二絕緣結構230b彼此實體連接而形成一連續性的結構。因此,第二絕緣結構230a與第一絕緣結構230a係構成一梳子狀的絕緣結構,且第二絕緣結構230b係作為梳子狀絕緣結構的梳柄;第一絕緣結構230a則作為梳子狀絕緣結構的梳齒。 Please also refer to Figures 5 to 7. The gate 220 of the HVMOS transistor device 200 provided in the preferred embodiment includes a gate conductive layer 222, a gate dielectric layer 224, and a sidewall spacer 226 formed on the sidewall of the gate conductive layer 222. And as shown in FIG. 5, is provided on the substrate 202 on the gate electrode lines 220 a extend along a first direction D 1. In addition, a plurality of STIs 204 for electrically isolating the HV MOS transistor component 200 from other semiconductor components are disposed in the substrate 202. It should be noted that the HV MOS transistor component 200 provided by the preferred embodiment further includes a plurality of insulating structures 230, such as a plurality of STIs. It should be noted that the insulating structure 230 provided by the preferred embodiment is composed of a first insulating structure 230a and a second insulating structure 230b, respectively. As shown in FIG. 5, each of the insulating structure 230a of the first insulating structure 230 along a second line extending direction D 2, D 2 and the second direction line as shown in FIG. 5, the first direction D 1 are staggered, Preferably they are perpendicular to each other. More importantly, the first insulating structure 230a is inserted into the n-type drift region 206, so that where the gate 220 passes, a pattern in which the n-type drift region 206 and the plurality of first insulating structures 230a are alternately arranged is formed. And the n-type drift region 206 and the first insulating structure 230a are staggered in the first direction D 1 . In other words, the gate 220 covers a portion of each of the n-type drift regions 206 and a portion of the respective insulating structures 230, and the drift regions 206 under the gates 220 and the first insulating structures 230 are staggered with each other along the first direction D 1 . As shown in FIG. 5, in the preferred embodiment, the first insulating structure 230a and the n-type drift region 106 have the same width, but are not limited thereto. The second insulating structure 230b of the insulating structure 230 extends along the first direction D 1 and is disposed below the gate 220 near one side of the drain region 212. In addition, as shown in FIG. 5, the second insulating structure 230b is disposed on one side of the first insulating structure 230a, and overlaps with a portion of each of the first insulating structures 230a and is physically connected. More importantly, each of the second insulating structures 230b is physically connected to each other to form a continuous structure. Therefore, the second insulating structure 230a and the first insulating structure 230a form a comb-like insulating structure, and the second insulating structure 230b serves as a comb handle of the comb-like insulating structure; the first insulating structure 230a serves as a comb-like insulating structure. Comb teeth.

請參閱第5圖與第7圖。在本較佳實施例中,係可藉由不同的製作方式形成STI 204與絕緣結構230。舉例來說,首先可於基底202上形成一淺溝渠(圖未示),用以預定第二絕緣結構230b形成之位置。隨後在基底202形成一圖案 化遮罩(圖未示),用以定義第一絕緣結構230a與STI 204的形成位置。接下來再進行一蝕刻製程,透過圖案化遮罩蝕刻基底202,以於基底202內形成深溝渠(圖未示)。隨後再於淺溝渠與各深溝渠內填入絕緣材料,並藉由一平坦化製程移除多餘的絕緣材料,而同時形成第一絕緣結構230a、第二絕緣結構230b與用以電性隔離HV MOS元件200與其他元件的STI 204。如第7圖所示,由於部分的第一絕緣結構230a係與第二絕緣結構230b重疊,因此在進行深溝渠的蝕刻製程時,該等重疊的部分即獲得較大的深度,故最後形成的第一絕緣結構230a亦可包含一第一部232與一第二部234。如第6圖所示,本較佳實施例中,第一部232之深度與STI 204之深度相同,而第二部234之深度則大於STI 204之深度。另外第二絕緣結構230b的深度則如第7圖所示,小於第一絕緣結構230a與STI 204,且較佳更小於汲極區域212的深度。然而,熟習該項技藝之人士應知,STI 204、第一絕緣結構230a與第二絕緣結構230b之形成方式係不限於上述之步驟,也可以分別製作之。因此在其他的實施例中,第一絕緣結構230a可以是本身不具有深度差異的結構,即第一絕緣結構230a具有一完全相同的深度,且該深度等於STI 204之深度。 Please refer to Figure 5 and Figure 7. In the preferred embodiment, the STI 204 and the insulating structure 230 can be formed by different fabrication methods. For example, a shallow trench (not shown) may be formed on the substrate 202 to predetermine the location where the second insulating structure 230b is formed. A pattern is then formed on the substrate 202 A mask (not shown) is used to define the formation positions of the first insulating structure 230a and the STI 204. Next, an etching process is performed to etch the substrate 202 through the patterned mask to form a deep trench (not shown) in the substrate 202. Then, the insulating material is filled in the shallow trench and the deep trenches, and the excess insulating material is removed by a planarization process, and the first insulating structure 230a and the second insulating structure 230b are simultaneously formed to electrically isolate the HV. STI 204 of MOS component 200 and other components. As shown in FIG. 7, since a part of the first insulating structure 230a overlaps with the second insulating structure 230b, when the etching process of the deep trench is performed, the overlapping portions obtain a large depth, so the final formed The first insulating structure 230a can also include a first portion 232 and a second portion 234. As shown in FIG. 6, in the preferred embodiment, the depth of the first portion 232 is the same as the depth of the STI 204, and the depth of the second portion 234 is greater than the depth of the STI 204. In addition, the depth of the second insulating structure 230b is smaller than the first insulating structure 230a and the STI 204, and preferably smaller than the depth of the drain region 212, as shown in FIG. However, those skilled in the art should be aware that the manner in which the STI 204, the first insulating structure 230a, and the second insulating structure 230b are formed is not limited to the above steps, and may be separately fabricated. Therefore, in other embodiments, the first insulating structure 230a may be a structure that does not have a depth difference by itself, that is, the first insulating structure 230a has an exact same depth, and the depth is equal to the depth of the STI 204.

請重新參閱第7圖。在本較佳實施例中,閘極導電層222重疊了部分p型基體區域208而形成一通道區域228,通道 區域228係具有一長度L1。此外閘極220亦與部分n型漂移區域206重疊且直接接觸,且閘極導電層222與n型漂移區域206重疊且直接接觸的部分具有一長度L2。另外閘極導電層222更與部分第二絕緣結構230b重疊,且該重疊的部分具有一長度L3。如第6圖所示,通道區域228與第二絕緣結構230b係藉由n型漂移區域206彼此分隔。更重要的是,在本較佳實施例中,長度L1、長度L2與長度L3任一者不可為零。由於第二絕緣結構230b的深度小於STI 204的深度,因此電場集中(electric field crowding)的現象可被減輕,故可在不增加導通電阻的情況下提升崩潰電壓。 Please refer back to Figure 7. In the preferred embodiment, the gate conductive layer 222 overlaps a portion of the p-type body region 208 to form a channel region 228 having a length L 1 . In addition, the gate 220 also overlaps and is in direct contact with the portion of the n-type drift region 206, and the portion of the gate conductive layer 222 that overlaps with the n-type drift region 206 and directly contacts has a length L 2 . In addition, the gate conductive layer 222 further overlaps a portion of the second insulating structure 230b, and the overlapped portion has a length L 3 . As shown in FIG. 6, the channel region 228 and the second insulating structure 230b are separated from each other by the n-type drift region 206. More importantly, in the preferred embodiment, either length L 1 , length L 2 , and length L 3 may not be zero. Since the depth of the second insulating structure 230b is smaller than the depth of the STI 204, the phenomenon of electric field crowding can be alleviated, so that the breakdown voltage can be increased without increasing the on-resistance.

請重新參閱第5圖至第7圖。閘極220下方係交錯形成有n型漂移區域206(以及形成於其內的部分p型基體區域208)與絕緣結構230。如第6圖所示,當閘極2120下方形成者為絕緣結構230的第一絕緣結構230a時,整個閘極結構的閘極導電層222與閘極介電層224係如第6圖所示與第一絕緣結構230a重疊。換句話說,本來可形成通道區的部分現在全部被第一絕緣結構230佔據。然而,當閘極220下方形成者係如第7圖所示為絕緣結構230的第二絕緣結構230b、n型漂移區域206以及部分p型基體區域208時,仍可保有通道區域228,並可確保電流可經由與n型漂移區域206與通道區域228自汲極區域212到達源極區域210,並在此路徑中達到壓降的目的。更重要的是,由於在平行第二 方向D2上,各n型漂移區域206兩側係如第5圖與第6圖所示皆設置有第一絕緣結構230a,故可減輕n型漂移區域206部分的電場,達到提升崩潰電壓的目的。此外,由於p型基體區域208的角落處(如第7圖中圓圈C所標示)係為最脆弱的p-n交界處,因此第一絕緣結構230a之深度較佳為大於p型基體區域208之深度,故可從兩側夾住p型基體區域208的角落C,而增強其電場,避免HV MOS電晶體元件200在p型基體區域208的角落C發生崩潰。 Please refer back to Figures 5 to 7. Below the gate 220, an n-type drift region 206 (and a portion of the p-type body region 208 formed therein) and an insulating structure 230 are interleaved. As shown in FIG. 6, when the first insulating structure 230a of the insulating structure 230 is formed under the gate 2120, the gate conductive layer 222 and the gate dielectric layer 224 of the entire gate structure are as shown in FIG. It overlaps with the first insulating structure 230a. In other words, the portion of the channel region that would otherwise be formed is now fully occupied by the first insulating structure 230. However, when the underlying formation of the gate 220 is the second insulating structure 230b of the insulating structure 230, the n-type drift region 206, and the partial p-type base region 208 as shown in FIG. 7, the channel region 228 can still be retained, and Ensuring that current can reach the source region 210 from the drain region 212 via the n-type drift region 206 and the channel region 228, and achieve a voltage drop in this path. More importantly, since the first insulating structure 230a is disposed on both sides of the n-type drift region 206 as shown in FIGS. 5 and 6 in the parallel second direction D 2 , the n-type drift region can be alleviated. The electric field in part 206 reaches the purpose of increasing the breakdown voltage. In addition, since the corner of the p-type base region 208 (as indicated by the circle C in FIG. 7) is the most fragile pn junction, the depth of the first insulating structure 230a is preferably greater than the depth of the p-type base region 208. Therefore, the corner C of the p-type base region 208 can be sandwiched from both sides to enhance the electric field thereof, thereby preventing the HV MOS transistor element 200 from collapsing at the corner C of the p-type base region 208.

因此,根據本較佳實施例所提供的HV MOS電晶體元件200,係藉由閘極220下方設置的第二絕緣結構230b減輕電場集中的現象,更藉由閘極220下方交錯設置的n型漂移區域206與第一絕緣結構230a減輕n型漂移區域206電場,故可在不增加導通電阻的前提下更提升崩潰電壓。 Therefore, the HV MOS transistor element 200 according to the preferred embodiment reduces the phenomenon of electric field concentration by the second insulating structure 230b disposed under the gate 220, and is further arranged by the n-type staggered under the gate 220. The drift region 206 and the first insulating structure 230a mitigate the electric field of the n-type drift region 206, so that the breakdown voltage can be further increased without increasing the on-resistance.

另外請參閱第8圖,第8圖為本發明所提供之HV MOS電晶體元件之一第三較佳實施例之部分佈局圖案示意圖。值得注意的是,為凸顯較佳實施例所提供之HV MOS電晶體元件某些組成元件的相對關係,摻雜區域如源極區域、汲極區域與基體區域等不再繪示於第8圖中。然而,熟習該項技藝之人士應可根據前述的第一與第二較佳實施例輕易思及該等組成元素的形成位置。 Please refer to FIG. 8. FIG. 8 is a partial layout diagram of a third preferred embodiment of the HV MOS transistor component provided by the present invention. It should be noted that in order to highlight the relative relationship of some constituent elements of the HV MOS transistor component provided by the preferred embodiment, the doped regions such as the source region, the drain region and the substrate region are not shown in FIG. 8 . in. However, those skilled in the art should readily appreciate the formation positions of the constituent elements in accordance with the first and second preferred embodiments described above.

請參閱第8圖。本較佳實施例所提供之HV MOS電晶體元件300包含一設置於一基底(圖未示)內的n型漂移區域域306,與一設置於n型漂移區域306上的閘極320,且閘極320係具有一操場跑道(racetrack)型的佈局形狀。如第8圖所示,閘極320係由一對互相平行的直線部分(liner portion)320a與一對分別設置於閘極直線部分320a兩端的曲線部分(curved end portion)320b所構成。另外,本較佳實施例所提供之閘極320亦可為任何用於HV MOS電晶體元件的圖案,舉例來說,閘極320可為一矩形框圖案,或沿一梳子圖形邊緣延伸而具有梳子框形狀。另外需注意的是,本較佳實施例所提供之HV MOS電晶體元件300可採用共用汲極(common source)或共用源極(common source)之設計。當HV MOS電晶體元件300採用共用源極設計時,源極區域係形成於跑道形狀的閘極320中央的n型漂移區域306內,也就是說共用源極係由閘極320所包圍環繞。同理當HV MOS電晶體元件300採用共用汲極設計時,汲極區域係形成於跑道形狀的閘極320中央的n型漂移區域域306內,故共用汲極被閘極320包圍環繞。 Please refer to Figure 8. The HV MOS transistor element 300 of the preferred embodiment includes an n-type drift region 306 disposed in a substrate (not shown) and a gate 320 disposed on the n-type drift region 306, and The gate 320 has a layout shape of a playground track type. As shown in Fig. 8, the gate 320 is composed of a pair of mutually parallel straight portions 320a and a pair of curved end portions 320b respectively provided at both ends of the gate straight portion 320a. In addition, the gate 320 provided in the preferred embodiment may also be any pattern for the HV MOS transistor component. For example, the gate 320 may be a rectangular frame pattern or extend along an edge of a comb pattern. Comb box shape. It should be noted that the HV MOS transistor component 300 provided by the preferred embodiment may adopt a design of a common source or a common source. When the HV MOS transistor element 300 is of a common source design, the source region is formed in the n-type drift region 306 at the center of the raceway-shaped gate 320, that is, the common source is surrounded by the gate 320. Similarly, when the HV MOS transistor element 300 is of a common drain design, the drain region is formed in the n-type drift region 306 at the center of the raceway-shaped gate 320, so that the common drain is surrounded by the gate 320.

本較佳實施例所提供之HV MOS電晶體元件300更包含一用以提供電性隔離的STI 304。此外值得注意的是,本較佳實施例所提供之HV MOS電晶體元件300更包含複數個絕緣結構330,例如複數個STI。絕緣結構330之一深度可具 有多種型態。舉例來說,絕緣結構330之深度可如第一較佳實施例所述以及第4圖所示,與STI 304相同。然而絕緣結構330亦可如第二較佳實施例所述,具有一第一絕緣結構與一第二絕緣結構,其中第一絕緣結構之深度係大於等於STI304之深度,而第二絕緣結構之深度係可如第6圖所示,小於第一絕緣結構與STI 304。此外,第一絕緣結構亦可如第二較佳實施例所述以及第6圖所示,又更包含了深度不同的第一部與第二部。上述深度差異變化係可參考前述之第一與第二較佳實施例,故於此係不再贅述。此外,當絕緣結構330包含具有深度差異的第一絕緣結構與第二絕緣結構時,深度小於第一絕緣結構以及其他STI的第二絕緣結構係設置於閘極320下方靠近共用汲極之一側。 The HV MOS transistor component 300 provided by the preferred embodiment further includes an STI 304 for providing electrical isolation. In addition, it is noted that the HV MOS transistor component 300 provided by the preferred embodiment further includes a plurality of insulating structures 330, such as a plurality of STIs. One of the insulating structures 330 may have a depth There are many types. For example, the depth of the insulating structure 330 can be the same as that of the STI 304 as described in the first preferred embodiment and in FIG. However, the insulating structure 330 can also have a first insulating structure and a second insulating structure as described in the second preferred embodiment, wherein the depth of the first insulating structure is greater than or equal to the depth of the STI 304, and the depth of the second insulating structure. The system can be smaller than the first insulating structure and the STI 304 as shown in FIG. In addition, the first insulating structure may also include the first portion and the second portion having different depths as described in the second preferred embodiment and the sixth embodiment. For the above-mentioned differences in depth differences, reference may be made to the first and second preferred embodiments described above, and thus no further details are provided herein. In addition, when the insulating structure 330 includes the first insulating structure and the second insulating structure having different depths, the second insulating structure having a depth smaller than the first insulating structure and other STIs is disposed under the gate 320 near one side of the shared drain .

請繼續參閱第8圖。值得注意的是,在本較佳實施例中各絕緣結構330排列方向係與閘極320延伸方向相同。更重要的是,絕緣結構330係穿插於n型漂移區域306內,因此在閘極320經過之處,係形成複數個n型漂移區域306與複數個絕緣結構330交錯設置的型態。在本較佳實施例中,在閘極直線部分320a下方的絕緣結構330與n型漂移區域306係具有相同的寬度,但不限於此。然而,在閘極曲線部分320b下方的絕緣結構330與n型漂移區域306可具有不同的寬度。更重要的是,在閘極曲線部分320b下方的各絕緣結構330本身可具有不同的寬度。如第8圖所示,閘極曲線部分 320b下方的絕緣結構330具有一第一端332與一第二端334,第一端332具有一寬度W1,第二端334具有一寬度W2,且寬度W1小於寬度W2。這是由於在閘極曲線部分320b常發生電場集中而降低崩潰電壓等狀況,因此本較佳實施例係於閘極曲線部分320b提供寬度更大的絕緣結構330,以減輕該部分電場集中的效應。 Please continue to see Figure 8. It should be noted that in the preferred embodiment, the insulating structures 330 are arranged in the same direction as the gate 320 extends. More importantly, the insulating structure 330 is inserted into the n-type drift region 306. Therefore, where the gate 320 passes, a pattern in which a plurality of n-type drift regions 306 and a plurality of insulating structures 330 are alternately disposed is formed. In the preferred embodiment, the insulating structure 330 under the gate straight portion 320a has the same width as the n-type drift region 306, but is not limited thereto. However, the insulating structure 330 and the n-type drift region 306 under the gate curve portion 320b may have different widths. More importantly, the respective insulating structures 330 under the gate curve portion 320b may themselves have different widths. As shown in FIG. 8, the insulating structure 330 under the gate curve portion 320b has a first end 332 and a second end 334. The first end 332 has a width W 1 and the second end 334 has a width W 2 . And the width W 1 is smaller than the width W 2 . This is because the electric field concentration is often caused in the gate curve portion 320b to reduce the breakdown voltage and the like. Therefore, the preferred embodiment provides the insulating structure 330 having a larger width in the gate curve portion 320b to alleviate the effect of the electric field concentration in the portion. .

由第8圖可知,閘極320下方係交錯形成有n型漂移區域306與絕緣結構330。當閘極320下方形成者為絕緣結構330時,整個閘極320與絕緣結構330重疊。換句話說,本來可形成通道區的部分現在全部被絕緣結構330佔據。然而,當閘極320下方形成者係如第8圖所示為n型漂移區域306時,仍可保有通道區,並可確保電子可經由通道區與n型漂移區域306自源極區域到達汲極區域,並在此路徑中達到壓降的目的。 As can be seen from FIG. 8, the n-type drift region 306 and the insulating structure 330 are alternately formed under the gate 320. When the insulator 320 is formed below the gate 320, the entire gate 320 overlaps the insulating structure 330. In other words, the portion of the channel region that would otherwise be formed is now fully occupied by the insulating structure 330. However, when the underlying formation of the gate 320 is the n-type drift region 306 as shown in FIG. 8, the channel region can still be preserved, and electrons can be ensured from the source region via the channel region and the n-type drift region 306. The polar region and the purpose of achieving pressure drop in this path.

因此,根據本第三較佳實施例所提供的HV MOS電晶體元件300,係藉由閘極320下方交錯設置的n型漂移區域306與絕緣結構330減輕n型漂移區域306的電場。此外當絕緣結構330包含了深度小於一般STI 304的絕緣結構時,更可減輕電場集中的現象。故本較佳實施例所提供的HV MOS電晶體元件300係可在不增加導通電阻的前提下更提升崩潰電壓。 Therefore, the HV MOS transistor element 300 according to the third preferred embodiment reduces the electric field of the n-type drift region 306 by the n-type drift region 306 and the insulating structure 330 staggered under the gate 320. In addition, when the insulating structure 330 includes an insulating structure having a depth smaller than that of the general STI 304, the phenomenon of electric field concentration can be alleviated. Therefore, the HV MOS transistor element 300 provided in the preferred embodiment can increase the breakdown voltage without increasing the on-resistance.

縱上所述,本發明所提供之HV MOS電晶體元件係提供了一設置於閘極下方,且與漂移區域交錯設置的絕緣結構,並藉由此交錯設置的漂移區域與絕緣結構減輕漂移區域的電場強度。此外當絕緣結構本身具有深度差異時,本發明更可藉由深度小於一般提供電性隔離的STI的淺絕緣結構減輕電場集中的效應。故本發明可克服低導通電阻以及高崩潰電壓,且這兩個要求常常是彼此衝突難以權衡的問題,在不增加導通電阻的前提下,有效地提升崩潰電壓,更增加HV MOS電晶體元件的能力。此外,本發明所提供的HV MOS電晶體元件更可有效地應用於共用源極或共用汲極之設計,並藉由在容易發生電場集中的部分提供寬度不同的絕緣結構,本發明所提供的HV MOS電晶體元件更可有效地減輕於共用源極或共用汲極設計常發生的電場集中造成崩潰電壓下降的問題。 In the above, the HV MOS transistor component provided by the present invention provides an insulating structure disposed under the gate and interleaved with the drift region, and the drift region and the insulating structure are used to reduce the drift region. Electric field strength. In addition, when the insulating structure itself has a difference in depth, the present invention can alleviate the effect of electric field concentration by a shallow insulating structure having a depth smaller than that of an STI generally providing electrical isolation. Therefore, the present invention can overcome low on-resistance and high breakdown voltage, and these two requirements are often difficult to balance with each other, and effectively increase the breakdown voltage without increasing the on-resistance, and further increase the HV MOS transistor component. ability. In addition, the HV MOS transistor element provided by the present invention can be effectively applied to a common source or a common drain design, and provides an insulating structure having a different width in a portion where electric field concentration is likely to occur, and the present invention provides The HV MOS transistor component is more effective in mitigating the problem of a breakdown voltage caused by a common source or common electric field concentration of a common drain design.

以上所述僅為本發明之較佳實施例,凡依本發明申請專利範圍所做之均等變化與修飾,皆應屬本發明之涵蓋範圍。 The above are only the preferred embodiments of the present invention, and all changes and modifications made to the scope of the present invention should be within the scope of the present invention.

10‧‧‧高壓橫向雙擴散金氧半導體電晶體元件 10‧‧‧High voltage lateral double diffused MOS transistor components

12‧‧‧半導體基底 12‧‧‧Semiconductor substrate

14‧‧‧源極 14‧‧‧ source

16‧‧‧閘極 16‧‧‧ gate

18‧‧‧汲極 18‧‧‧汲polar

20‧‧‧P型井 20‧‧‧P type well

22‧‧‧P型摻雜區 22‧‧‧P-doped area

30‧‧‧N型井 30‧‧‧N type well

40‧‧‧閘極介電層 40‧‧‧ gate dielectric layer

42‧‧‧場氧化層 42‧‧‧Field oxide layer

100、200、300‧‧‧高壓金氧半導體電晶體元件 100, 200, 300‧‧‧ high voltage MOS transistor components

102、202‧‧‧基底 102, 202‧‧‧ base

104、204、304‧‧‧淺溝隔離 104, 204, 304‧‧‧ shallow trench isolation

106、206、306‧‧‧n型漂移區域 106, 206, 306‧‧‧n drift zone

108、208‧‧‧p型基體區域 108, 208‧‧‧p type base area

110、210‧‧‧源極區域 110, 210‧‧‧ source area

112、212‧‧‧汲極區域 112, 212‧‧ ‧ bungee area

114、214‧‧‧p型摻雜區 114, 214‧‧‧p-type doped region

120、220、320‧‧‧閘極 120, 220, 320‧‧‧ gate

320a‧‧‧直線部分 320a‧‧‧ Straight line

320b‧‧‧曲線部分 320b‧‧‧ Curve section

122、222‧‧‧閘極導電層 122, 222‧‧‧ gate conductive layer

124、224‧‧‧閘極介電層 124, 224‧‧ ‧ gate dielectric layer

126、226‧‧‧側壁子 126, 226‧‧‧ side wall

128、228‧‧‧通道區 128, 228‧‧‧ passage area

130、230、330‧‧‧絕緣結構 130, 230, 330‧‧‧ insulation structure

230a‧‧‧第一絕緣結構 230a‧‧‧First insulation structure

230b‧‧‧第二絕緣結構 230b‧‧‧Second insulation structure

232‧‧‧第一部 232‧‧‧ first

234‧‧‧第二部 234‧‧‧Part II

332‧‧‧第一端 332‧‧‧ first end

334‧‧‧第二端 334‧‧‧ second end

A1-A1’、A2-A2’、B1-B1’、B2-B2’‧‧‧切線 A 1 -A 1 ', A 2 -A 2', B 1 -B 1 ', B 2 -B 2' ‧‧‧ tangent

C‧‧‧基體區域角落 C‧‧‧ Corner of the base area

D1‧‧‧第一方向 D 1 ‧‧‧First direction

D2‧‧‧第二方向 D 2 ‧‧‧second direction

L1、L2、L3‧‧‧長度 L 1 , L 2 , L 3 ‧‧‧ length

W1、W2‧‧‧寬度 W 1 , W 2 ‧ ‧ width

第1圖為一習知HV-LDMOS電晶體元件之剖面示意圖。 Figure 1 is a schematic cross-sectional view of a conventional HV-LDMOS transistor device.

第2圖為本發明所提供之HV MOS電晶體元件之第一較佳實施例之部分佈局圖案示意圖。 2 is a partial layout diagram of a first preferred embodiment of the HV MOS transistor component provided by the present invention.

第3圖至第4圖分別為第2圖中沿A1-A1’與B1-B1’切線所獲得之剖面示意圖。 Fig. 3 to Fig. 4 are schematic cross-sectional views taken along line A 1 - A 1 ' and B 1 - B 1 ' in Fig. 2, respectively.

第5圖為本發明所提供之HV MOS電晶體元件之一第二較佳實施例之部分佈局圖案示意圖。 FIG. 5 is a partial layout diagram of a second preferred embodiment of the HV MOS transistor component provided by the present invention.

第6圖至第7圖分別為第5圖中沿A2-A2’與B2-B2’切線所獲得之剖面示意圖。 Fig. 6 to Fig. 7 are schematic cross-sectional views taken along line A 2 - A 2 ' and B 2 - B 2 ' in Fig. 5, respectively.

第8圖為本發明所提供之HV MOS電晶體元件之一第三較佳實施例之部分佈局圖案示意圖。 FIG. 8 is a partial layout diagram of a third preferred embodiment of the HV MOS transistor component provided by the present invention.

100‧‧‧高壓金氧半導體電晶體元件 100‧‧‧High voltage MOS transistor components

104‧‧‧淺溝隔離 104‧‧‧Shallow trench isolation

106‧‧‧n型漂移區域 106‧‧‧n type drift zone

120‧‧‧閘極 120‧‧‧ gate

130‧‧‧絕緣結構 130‧‧‧Insulation structure

A1-A1’‧‧‧切線 A 1 -A 1 '‧‧‧ Tangent

B1-B1’‧‧‧切線 B 1 -B 1 '‧‧‧ Tangent

D1‧‧‧第一方向 D 1 ‧‧‧First direction

D2‧‧‧第二方向 D 2 ‧‧‧second direction

Claims (16)

一種高壓半導體電晶體元件(high voltage metal-oxide-semiconductor,HV MOS)電晶體元件,包含有:一基底;一閘極,設置於該基底上;一汲極區域與一源極區域,分別設置於該閘極兩側之該基底內;一基體區域(body region)與一漂移區域(drift region),其中該源極區域設置於該基體區域中,且該基體區域與該汲極區域係設置於該漂移區域中;以及一第一絕緣結構(isolation structure),設置於該閘極下方,且該閘極係完全重疊於該第一絕緣結構。 A high voltage metal-oxide-semiconductor (HV MOS) transistor component includes: a substrate; a gate disposed on the substrate; a drain region and a source region, respectively In the substrate on both sides of the gate; a body region and a drift region, wherein the source region is disposed in the substrate region, and the substrate region and the drain region are disposed In the drift region; and a first isolation structure disposed under the gate, and the gate is completely overlapped with the first insulation structure. 如申請專利範圍第1項所述之HV MOS電晶體元件,更包含複數個第二絕緣結構,設置於該基底內,該等第二絕緣結構係電性絕緣該HV MOS電晶體元件。 The HV MOS transistor device of claim 1, further comprising a plurality of second insulating structures disposed in the substrate, the second insulating structures electrically insulating the HV MOS transistor. 如申請專利範圍第2項所述之HV MOS電晶體元件,其中該第一絕緣結構之一深度係等於該等第二絕緣結構之一深度。 The HV MOS transistor component of claim 2, wherein one of the first insulating structures has a depth equal to one of the second insulating structures. 如申請專利範圍第2項所述之HV MOS電晶體元件,其中該第一絕緣結構更包含一第一部與一第二部,該第一部包 含一第一深度,而該第二部包含一第二深度。 The HV MOS transistor component of claim 2, wherein the first insulating structure further comprises a first portion and a second portion, the first portion A first depth is included and the second portion includes a second depth. 如申請專利範圍第4項所述之HV MOS電晶體元件,其中該第一深度係等於該第二絕緣結構之一深度,該第二深度係大於該第二絕緣結構之一該深度。 The HV MOS transistor component of claim 4, wherein the first depth is equal to a depth of the second insulating structure, and the second depth is greater than the depth of one of the second insulating structures. 如申請專利範圍第2項所述之HV MOS電晶體元件,更包含一第三絕緣結構,設置於該閘極下方。 The HV MOS transistor component of claim 2, further comprising a third insulating structure disposed under the gate. 如申請專利範圍第6項所述之HV MOS電晶體元件,其中該第三絕緣結構之一深度係小於該第一絕緣結構之一深度與該等第二絕緣結構之一深度。 The HV MOS transistor component of claim 6, wherein a depth of one of the third insulating structures is less than a depth of one of the first insulating structures and a depth of the second insulating structures. 申請專利範圍第6項所述之HV MOS電晶體元件,其中該閘極係覆蓋部分該第三絕緣結構。 The HV MOS transistor component of claim 6, wherein the gate portion covers a portion of the third insulating structure. 申請專利範圍第6項所述之HV MOS電晶體元件,其中該第一絕緣結構係接觸該第三絕緣結構。 The HV MOS transistor component of claim 6, wherein the first insulating structure contacts the third insulating structure. 一種高壓半導體電晶體元件(HV MOS)電晶體元件,包含有:一基底;一閘極,設置於該基底上,且該閘極係沿一第一方向延 伸;複數個漂移區域,形成於該基底內,且該等漂移區域係沿該第一方向排列;複數個第一絕緣結構,形成於該基底內,各該第一絕緣結構係沿一第二方向延伸,且該第二方向垂直於該第一方向,該等第一絕緣結構係沿該第一方向排列;以及一第二絕緣結構,設置於該基底內,且沿該第一方向延伸,且該閘極與該第二絕緣結構部分重疊,其中該閘極係覆蓋部分各該漂移區域與部分各該第一絕緣結構,且該閘極下方之該等漂移區域與該等第一絕緣結構係沿該第一方向彼此交錯排列。 A high voltage semiconductor transistor component (HV MOS) transistor component includes: a substrate; a gate disposed on the substrate, and the gate is extended along a first direction Extending; a plurality of drift regions are formed in the substrate, and the drift regions are arranged along the first direction; a plurality of first insulating structures are formed in the substrate, and each of the first insulating structures is along a second The direction is extended, and the second direction is perpendicular to the first direction, the first insulating structures are arranged along the first direction; and a second insulating structure is disposed in the substrate and extends along the first direction, And the gate partially overlaps the second insulating structure, wherein the gate covers the drift region and a portion of each of the first insulating structures, and the drift regions under the gate and the first insulating structures The lines are staggered with each other along the first direction. 如申請專利範圍第10項所述之HV MOS電晶體元件,其中該等漂移區域互相電性連接。 The HV MOS transistor component of claim 10, wherein the drift regions are electrically connected to each other. 如申請專利範圍第11項所述之HV MOS電晶體元件,更包含一源極區域與一汲極區域,設置於該閘極兩側之該漂移區域內。 The HV MOS transistor component of claim 11, further comprising a source region and a drain region disposed in the drift region on both sides of the gate. 如申請專利範圍第10項所述之HV MOS電晶體元件,其中該第二絕緣結構係與各該第一絕緣結構部分重疊。 The HV MOS transistor component of claim 10, wherein the second insulating structure partially overlaps each of the first insulating structures. 如申請專利範圍第10項所述之HV MOS電晶體元件, 其中該第二絕緣結構之一深度係小於該等第一絕緣結構之一深度。 For example, the HV MOS transistor component described in claim 10, Wherein the depth of one of the second insulating structures is less than a depth of the first insulating structures. 如申請專利範圍第10所述之HV MOS電晶體元件,其中各該第一絕緣結構包含一第一端與一第二端。 The HV MOS transistor component of claim 10, wherein each of the first insulating structures comprises a first end and a second end. 如申請專利範圍第15項所述之HV MOS電晶體元件,其中該第一端之寬度與該第二端之寬度不同。 The HV MOS transistor component of claim 15, wherein the width of the first end is different from the width of the second end.
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